enter npoints,number_propagators,rank,scaloop,muscale scaloop= 1 -> looptools 1-loop scaloop= 2 -> avh 1-loop (massive with complex masses) scaloop= 3 -> qcdloop 1-loop (Ellis and Zanderighi) muscale (dimension of energy) is the scale for the 1-loop integrals ------------------------------------------------------------------------ | You are using CutTools - Version 1.6.9 | | Authors: G. Ossola, C. Papadopoulos, R. Pittau | | Published in JHEP 0803:042,2008 | | http://www.ugr.es/~pittau/CutTools | | | | Internal mproutines detected in CutTools | ------------------------------------------------------------------------ ######################################################################## # # # You are using OneLOop-2.2 # # # # for the evaluation of 1-loop scalar 1-, 2-, 3- and 4-point functions # # # # author: Andreas van Hameren # # date: 04-07-2011 # # # # Please cite # # A. van Hameren, # # Comput.Phys.Commun. 182 (2011) 2427-2438, arXiv:1007.4716 # # A. van Hameren, C.G. Papadopoulos and R. Pittau, # # JHEP 0909:106,2009, arXiv:0903.4665 # # in publications with results obtained with the help of this program. # # # ######################################################################## ######################################################################## # # # You are using OneLOop in multiple precision # # # # obtained by R. Pittau (pittau@ugr.es) # # from the original OneLOop-2.2 package # # # # Internal mproutines detected. # # # ######################################################################## iter= 1 Complete Amplitude (without r2): finite part amp(0)= (-1.10581082351118079E-005, 3.82757143995054834E-005) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-1.10581082351118079E-005, 3.82757143995054834E-005) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 2 Complete Amplitude (without r2): finite part amp(0)= (-6.08823179391560724E-005,-1.22143014817594674E-004) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-6.08823179391560724E-005,-1.22143014817594674E-004) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 3 Complete Amplitude (without r2): finite part amp(0)= (-4.72115910175283397E-005, 1.14113770754292865E-004) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-4.72115910175283397E-005, 1.14113770754292865E-004) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 4 Complete Amplitude (without r2): finite part amp(0)= ( 2.70399434697404534E-005, 1.75049104459220527E-004) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 2.70399434697404534E-005, 1.75049104459220527E-004) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 5 Complete Amplitude (without r2): finite part amp(0)= (-2.07096851426084388E-006,-5.30949884696294093E-006) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-2.07096851426084388E-006,-5.30949884696294093E-006) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 6 Complete Amplitude (without r2): finite part amp(0)= (-2.11139839390537274E-005, 5.43370217248214911E-005) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-2.11139839390537274E-005, 5.43370217248214911E-005) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 7 Complete Amplitude (without r2): finite part amp(0)= ( 1.13085667228763524E-006,-1.29035666519133749E-005) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= ( 1.13085667228763524E-006,-1.29035666519133749E-005) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 8 Complete Amplitude (without r2): finite part amp(0)= (-5.99127706399224493E-006, 2.74144985550398823E-006) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-5.99127706399224493E-006, 2.74144985550398823E-006) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 9 Complete Amplitude (without r2): finite part amp(0)= (-6.40182901121604650E-006, 8.91217226231079370E-006) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-6.40182901121604650E-006, 8.91217226231079370E-006) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T iter= 10 Complete Amplitude (without r2): finite part amp(0)= (-8.88730499584883462E-006,-4.29134704900984671E-005) coeff of 1/eps pole amp(1)= ( 0.0000000000000000 , 0.0000000000000000 ) coeff of 1/eps^2 pole amp(2)= ( 0.0000000000000000 , 0.0000000000000000 ) ampcc= (-8.88730499584883462E-006,-4.29134704900984671E-005) R1= ( 0.0000000000000000 , 0.0000000000000000 ) stable= T n_tot = 10.000000000000000 n_mp = 0.0000000000000000 n_disc= 0